1999ApJ...526..957K


Query : 1999ApJ...526..957K

1999ApJ...526..957K - Astrophys. J., 526, 957-975 (1999/December-1)

The characteristics of millisecond pulsar emission. III. From low to high frequencies.

KRAMER M., LANGE C., LORIMER D.R., BACKER D.C., XILOURIS K.M., JESSNER A. and WIELEBINSKI R.

Abstract (from CDS):

In this paper we present the first observations of a large sample of millisecond pulsars at frequencies of 2.7 GHz (11 cm) and 4.9 GHz (6 cm). For almost all sources, these represent the first 11 cm observations ever. The new measurements more than double the number of millisecond pulsars studied at 6 cm. Our new flux measurements extend the known spectra for millisecond pulsars to the highest frequencies to date. The coverage of more than a decade of the radio spectrum allows us for the first time to search for spectral breaks, as so often observed in normal pulsars around 1 GHz. The results suggest that, unlike normal pulsars, millisecond pulsar spectra can be largely described by a single power law. We align the observed millisecond pulsar profiles with data from lower frequencies to search for indications of disturbed magnetic fields, and attempt to resolve questions that have been raised in recent literature. Deviations from a dipolar magnetic field structure are not evident, and absolute timing across the wide frequency range with a single dispersion measure is possible. We seem to observe mainly unfilled emission beams, which must originate from a very compact region. The existence of nondipolar field components therefore cannot be excluded. A compact emission region is also suggested by a remarkably constant profile width or component separation over a very wide frequency range. This observed difference from the emission properties of normal pulsars is highly significant. For a few sources, polarization data at 2.7 and 4.9 GHz could also be obtained that indicate that despite the typically larger degree of polarization at lower frequencies, millisecond pulsars are weakly polarized or even unpolarized at frequencies above 3 GHz. The simultaneous decrease in degree of polarization and the constant profile width thus question proposals that link depolarization and decreasing profile width for normal pulsars to the same propagation effect (i.e., birefringence). Comparing the properties of core and conal-like profile components to those of normal pulsars, we find less significant patterns in their spectral evolution for the population of millisecond pulsars. Hence, we suggest that core and conal emission may be created by the same emission process. Given the small change in profile width, the indicated depolarization of the radiation, and the possible simple flux density spectra, MSP emission properties tend to resemble those of normal pulsars, only shifted toward higher frequencies.

Abstract Copyright: ∼

Journal keyword(s): Polarization - Stars: Pulsars: General - Radiation Mechanisms: Nonthermal - radio continuum: stars - Stars: Evolution

CDS comments: p.964 : PSR B1831+04 misprint for 1831-04

Simbad objects: 23

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Number of rows : 23
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 PSR J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 365 2
2 PSR B0355+54 Psr 03 58 53.7165 +54 13 13.727           ~ 465 1
3 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
4 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
5 PSR J0621+10 Psr 06 21 22.11108 +10 02 38.7410           ~ 128 1
6 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
7 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
8 PSR J1022+10 Psr 10 22 57.990 +10 01 52.92           ~ 279 2
9 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
10 PSR J1045-45 Psr 10 45 50.179671 -45 09 54.05686           ~ 154 1
11 PSR B1257+12 Psr 13 00 03.1075 +12 40 55.155           ~ 546 1
12 PSR J1518+4904 Psr 15 18 16.832 +49 04 34.19           ~ 201 1
13 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
14 PSR B1620-26 Psr 16 23 38.2218 -26 31 53.769     21.30     ~ 318 2
15 PSR J1640+2224 Psr 16 40 16.744850 +22 24 08.84119           ~ 210 0
16 PSR J1643-1224 Psr 16 43 38.16612 -12 24 58.6334           ~ 260 2
17 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
18 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
19 PSR B1831-04 Psr 18 34 25.62100 -04 26 15.7000           ~ 103 0
20 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
21 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
22 NGC 7027 PN 21 07 01.571952 +42 14 10.47120   10.358 8.831 10.157   ~ 2541 1
23 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0

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